Probing Superatomic Orbitals of Sc-Doped and Undoped Silver Cluster Anions via Photoelectron Angular Anisotropy.

Valence s electrons in alkali- or coinage-metal clusters are conceived to delocalize over the metal frameworks. The electrons occupy so-called superatomic orbitals (SAOs, i.e., 1S, 1P, 1D, 2S, 1F, ...), which provide an essential picture for understanding the size-dependent, unique properties of these metal clusters. While such electronic shells are unambiguously identified in their photoelectron spectra and supported by electronic structure calculations, characterization of SAOs in heteroatom-doped metal clusters has remained elusive as the doping significantly affects its energy levels and even alters the ordering of SAOs. Here, we present a photoelectron imaging study to explore SAOs formed in Sc-doped and undoped silver cluster anions, AgNSc- (N = 15, 16) and AgN- (N = 18, 19). Photoelectron angular distributions from their outermost SAOs are clearly visualized, whose characters are analyzed with the aid of density functional theory calculations. The present methodology enables us to explore not only the quantized energy levels but also the spatial distributions of SAOs formed in various metal cluster anions.

Large orbital magnetic moments of small, free cobalt cluster ions Co[Formula: see text] with n [Formula: see text].

The size dependent electronic structure and separate spin and orbital magnetic moments of free Co[Formula: see text] ([Formula: see text]) cluster ions have been investigated by x-ray absorption and x-ray magnetic circular dichroism spectroscopy in a cryogenic ion trap. A very large orbital magnetic moment of [Formula: see text] per atom was determined for Co[Formula: see text], which is one order of magnitude larger than in the bulk metal. Large orbital magnetic moments per atom of ≈1 [Formula: see text] were also found for Co[Formula: see text], Co[Formula: see text], and Co[Formula: see text]. The orbital contribution to the total magnetic moment shows a non-monotonic cluster size dependence: The orbital contribution increases from a local minimum at n = 2 to a local maximum at n = 5 and then decreases with increasing cluster size. The 3d spin magnetic moment per atom is nearly constant and is solely defined by the number of 3d holes which shows that the 3d majority spin states are fully occupied, that is, 3d hole spin polarization is 100%.

Electronic ground state of Ni2.

The Φ9/24 ground state of the Ni2+ diatomic molecular cation is determined experimentally from temperature and magnetic-field-dependent x-ray magnetic circular dichroism spectroscopy in a cryogenic ion trap, where an electronic and rotational temperature of 7.4±0.2 K was reached by buffer gas cooling of the molecular ion. The contribution of the spin dipole operator to the x-ray magnetic circular dichroism spin sum rule amounts to 7Tz=0.17±0.06µB per atom, approximately 11% of the spin magnetic moment. We find that, in general, homonuclear diatomic molecular cations of 3d transition metals seem to adopt maximum spin magnetic moments in their electronic ground states.

Direct observation of high-spin states in manganese dimer and trimer cations by x-ray magnetic circular dichroism spectroscopy in an ion trap.

The electronic structure and magnetic moments of free Mn2 (+) and Mn3 (+) are characterized by 2p x-ray absorption and x-ray magnetic circular dichroism spectroscopy in a cryogenic ion trap that is coupled to a synchrotron radiation beamline. Our results directly show that localized magnetic moments of 5 µB are created by 3d(5)((6)S) states at each ionic core, which are coupled ferromagnetically to form molecular high-spin states via indirect exchange that is mediated in both cases by a delocalized valence electron in a singly occupied 4s derived antibonding molecular orbital with an unpaired spin. This leads to total magnetic moments of 11 µB for Mn2 (+) and 16 µB for Mn3 (+), with no contribution of orbital angular momentum.

Magnetic moments of chromium-doped gold clusters: the Anderson impurity model in finite systems.

The magnetic moment of a single impurity atom in a finite free electron gas is studied in a combined x-ray magnetic circular dichroism spectroscopy, charge transfer multiplet calculation, and density functional theory study of size-selected free chromium-doped gold clusters. The observed size dependence of the local magnetic moment can be understood as a transition from a local moment to a mixed valence regime. This shows that the Anderson impurity model essentially describes finite systems even though the discrete density of states introduces a significant deviation from a bulk metal, and the free electron gas is only formed by less than 10 electrons. Electronic shell closure in the gold host minimizes the interaction of localized impurity states with the confined free electron gas and preserves the magnetic moment of 5 µ_{B} fully in CrAu_{2}^{+} and almost fully in CrAu_{6}^{+}. Even for open-shell species, large local moments are observed that scale with the energy gap of the gold cluster. This indicates that an energy gap in the free electron gas stabilizes the local magnetic moment of the impurity atom.

Electronic ground states of Fe2(+) and Co2(+) as determined by x-ray absorption and x-ray magnetic circular dichroism spectroscopy.

The (6)Π electronic ground state of the Co2 (+) diatomic molecular cation has been assigned experimentally by x-ray absorption and x-ray magnetic circular dichroism spectroscopy in a cryogenic ion trap. Three candidates, (6)Φ, (8)Φ, and (8)Γ, for the electronic ground state of Fe2 (+) have been identified. These states carry sizable orbital angular momenta that disagree with theoretical predictions from multireference configuration interaction and density functional theory. Our results show that the ground states of neutral and cationic diatomic molecules of 3d transition elements cannot generally be assumed to be connected by a one-electron process.

Spin coupling and orbital angular momentum quenching in free iron clusters.

Magnetic spin and orbital moments of size-selected free iron cluster ions Fe{n}{+} (n=3-20) have been determined via x-ray magnetic circular dichroism spectroscopy. Iron atoms within the clusters exhibit ferromagnetic coupling except for Fe{13}{+}, where the central atom is coupled antiferromagnetically to the atoms in the surrounding shell. Even in very small clusters, the orbital magnetic moment is strongly quenched and reduced to 5%-25% of its atomic value while the spin magnetic moment remains at 60%-90%. This demonstrates that the formation of bonds quenches orbital angular momenta in homonuclear iron clusters already for coordination numbers much smaller than those of the bulk.

Chromosomal assignment of LASP1 and LASP2 genes and organization of the LASP2 gene in chicken.

Lasp-1 and lasp-2 are actin-binding proteins that contain a LIM domain, two nebulin repeats and an SH3 domain with significant identity. We determined the chromosomal locations of the LASP1 and LASP2 genes in chicken by fluorescence in situ hybridization. The LASP1 gene was localized to a pair of microchromosomes and the LASP2 gene was localized to chromosome 2p3.1, indicating that the chromosomal locations of the LASP1 and LASP2 genes are highly conserved between chicken and human. The comparison of genomic and cDNA sequences of chicken lasp-2 and nebulette, a nebulin-related protein in muscle, suggested that both the corresponding mRNAs shared exons in the same manner as their human homologues. When compared with the domain structure of nebulette, another nebulin repeat was predicted for lasp-2, and all the nebulin repeats of lasp-2 were better conserved than those in nebulette. We also found the exon boundaries in nebulin repeats of lasp-2 were similar to those of other nebulin-related proteins.

[Factors influencing grief due to bereavement among elderly widows and widowers].

OBJECTIVES: To identify the factors that influence the grief of bereaved elderly people due to the death of a spouse. METHOD: Subjects consisted of 172 widows and widowers (137 females, 35 males) aged 60 or older who experienced bereavement of a spouse in the last three years. Between August 1994 and October 1996, the subjects were interviewed using a semi-structured questionnaire and data was also obtained from self-report measures which were returned by mail. A questionnaire consisting of 26 items was prepared based on the theories of Parkes and Deeken. These responses were classified into 4 categories (sensory paralysis, deep attachment and protest, disintegration, reconstruction) and analysis was made by these categories. The time course of the grief was evaluated at 1 week, 49 days and 1 year after the death of the spouse and the time of survey. RESULTS: (1) Of the 172 subjects, general health was graded as poor or slightly poor in 33.6%, 67.4% cared for their spouse during medical treatment; and the average GDS depression score was 5.85 (SD = 3.50). (2) With respect to anticipated grief, while their spouses were under medical treatment, more than 50% of the subjects were thinking "I will do Whatever I can to cope". (3) Change in grief response over time: For "sensory paralysis", "I have done whatever I can" rated the highest at 3 points or more on a scale of 4, from immediately after the spouse's death to the present. For "deep attachment and protest", deep attachment including "always thinking of the lost one" marked higher (3.4 points immediately after death to 2.9 at present) than protest. For "disintegration", "nobody understands what I feel" rated the highest (2.6-2.9 points). For "reconstruction", the subjects gradually accepted the death as "unavoidable" and had started to adapt. (4) Factors that significantly influenced grief were the subject's health condition, whether the subject had been notified of the name of the disease or given a prognosis; whether subject provided care for the spouse and GDS depression score. CONCLUSION: Sufficient anticipated grief resulted in a feeling of achievement in the sensory paralysis aspect of the grief response and in a long lasting feeling of deep attachment as loneliness and solitude. Disintegration was largely related to depression according to GDS score. Grief was less deeply felt when the subject was healthy, had been informed of the name of the spouse's disease, and had cared for the spouse during medical treatment before bereavement.

A 260-kDa filamin/ABP-related protein in chicken gizzard smooth muscle cells is a new component of the dense plaques and dense bodies of smooth muscle.

A 260-kDa protein, termed cgABP260, which localized in the dense plaques and dense bodies of smooth muscle cells, was found in a low-salt alkaline extract of chicken gizzard smooth muscle. An antibody against cgABP260 was used to screen a chicken gizzard cDNA library, and the nucleotide sequence of the partial cDNA encoding this protein was determined. Comparison of predicted amino acid sequences revealed that the protein had significant homology with human ABP-280 and chicken retina filamin [Barry, C.P. et al. (1993) J. Biol. Chem. 268, 25577-25586], but despite the high homology, cgABP260 was immunologically distinguishable from filamin. Immunoblot analysis showed that an anti-cgABP260 antibody reacted exclusively with the cgABP260 band of smooth, skeletal, and cardiac muscle tissues. By indirect immunofluorescence, the membrane-affinity-purified antibody against cgABP260 intensely stained the dense plaques of the isolated smooth muscle cells. Immunoelectron microscopy showed that immunogold particles representing cgABP260 were found abundantly on the dense plaques and less abundantly on the dense bodies. Its amino acid sequence, molecular size, immunological reactivity, and localization in smooth muscle thus indicated that cgABP260 is a new component of the dense plaques and dense bodies of smooth muscle cells.

Identification of actin-binding proteins from sea urchin eggs by F-actin affinity column chromatography.

Novel F-actin binding proteins of sea urchin eggs were searched for in order to study regulation of the actin cytoskeleton during fertilization and cell division. An extract of unfertilized eggs was analyzed by F-actin column chromatography. Several previously characterized F-actin-modulating proteins such as spectrin, myosin, and fascin bound to the column. The eluates from the column also contained proteins having apparent molecular weights of 225K, 150K, 70K, 60K, 45K, 40K, 38K, 36K, 34K, 20K, and 15K, which were thought to be novel cytoskeletal proteins judging from their molecular weights and non-reactivity to antibodies against previously characterized F-actin-modulating proteins. Most of the proteins in the F-actin column eluates co-sedimented with F-actin. Partial amino acid sequences of the peptides derived from the 45K and 40K proteins showed that these proteins are homologous to Arp3 and Arp2 subfamilies of actin-related proteins, respectively. The 150K protein seemed to be an unconventional myosin, that belongs to myosin VI subfamily. Amino acid sequences of two fragments from the 60K protein showed homology to that of coronin. The 150K protein was localized by immunofluorescence microscopy to the cleavage furrows in both whole cell sample and isolated cortex of dividing eggs. The 70K protein was uniformly localized in the cortical layer in the whole egg, but weak staining of the cleavage furrow region with the antiserum was observed in the isolated cortex. The 60K protein was localized to both the bulk cortical layer and the cleavage furrow, but the modes of localization were different.

A case of dyshormonogenetic goiter complicated with growth hormone deficiency.

A 17-year-old male patient with dyshormonogenetic goiter complicated with follicular adenoma and growth hormone deficiency is described. He had short stature (-2.3 SD), diffuse goiter and a particularly large nodule in the right lobe of the thyroid gland. The endocrinological studies revealed slight hypothyroidism. He underwent surgical removal of the tumor, diagnosed histopathologically as follicular adenoma, embryonal type; and the diffuse goiter was diagnosed as dyshormonogenetic goiter. It was speculated that long-term hypersecretion of thyroid stimulating hormone (TSH) caused adenoma in the thyroid gland. Although the goiter disappeared after oral thyroxine replacement therapy, his height gain remained poor. Then, he was diagnosed partial growth hormone deficiency, and growth hormone therapy improved his height gain. It has been reported that a high percentage of patients with congenital hypothyroidism have additional anomalies. This is, however, the first reported case of dyshormonogenetic goiter complicated with growth hormone deficiency.

A high molecular mass protein isolated from chicken gizzard: its localization at the dense plaques and dense bodies of smooth muscle and the Z-disks of skeletal muscle.

We purified a 450 kDa protein from a low-salt alkaline extract of chicken gizzard smooth muscle. This high molecular mass protein could be extracted with the low-salt alkaline solution at 37 degrees C but not at 4 degrees C. The 450 kDa protein was isolated from the extract by ammonium sulfate fractionation and following sequential column chromatography using hydroxylapatite, DEAE-Cellulofine A-800m and phenyl-Sepharose CL-4B resins. The partially purified protein molecule resembled a flexible rod with a globular head and an irregular-shaped tail. Its length was approximately 300 nm. The nucleotide sequence of the partial cDNA encoding this protein was determined and analyzed with a data base. The analysis showed that the protein revealed significant homology with the rod region of chicken filamin (57% homology in amino acid sequence). Immunoblot analysis showed that an affinity-purified antibody reacted exclusively with the 450 kDa protein band of smooth, skeletal and cardiac muscle tissues. By indirect immunofluorescence microscopy, we examined the localization of the 450 kDa protein in smooth and skeletal muscle cells. The affinity-purified antibody against the 450 kDa protein stained the dense plaques and dense bodies of smooth muscle, the peripheral region of Z-disks and the subsarcolemmal region of skeletal muscle. Immunoelectron microscopy confirmed the localization of the 450 kDa protein at the peripheral regions of the actin anchoring structures mentioned above. Judging from its amino acid sequence, molecular size, molecular shape, immunological reactivity and localization in muscle cells, the 450 kDa protein seemed to be a new component associated with the actin-anchoring structures of muscle tissues.(ABSTRACT TRUNCATED AT 250 WORDS)

A 36-kDa protein of the dense bodies of smooth muscle cells.

We purified a 36-kDa protein from a low-salt, alkaline extract of chicken gizzard smooth muscle by sequential column chromatography using DEAE-Cellurofine A-800 m, hydroxylapatite, and CM-Cellurofine C-500. This protein decreased the low-shear viscosity of actin filaments and coprecipitated with them by centrifugation at 18,500 x g. Electron microscopy showed that the 36-kda peptide bundled actin filaments. Immunoblot analysis revealed that an affinity-purified antibody against the 36-kDa protein reacted exclusively with the 36-kDa protein band of smooth muscle. In indirect immunofluorescence microscopy, the affinity-purified anti-36-kDa protein antibody stained the dotty structures of isolated smooth muscle cells, while in post-embedding immunoelectron microscopy, most of the colloidal gold particles representing the 36-kDa protein were found on the dense bodies of ultrathin sections of chicken gizzard smooth muscle cells. The antibody did not stain the dense plaques of isolated smooth muscle cells. Judging from its molecular weight, the 36-kDa protein is concluded to be a new component of the dense bodies of smooth muscle.

Induced phase modulation of chirped continuum pulses studied with a femtosecond frequency-domain interferometer.

The effect of rapid phase change on chirped continuum pulses is studied with a frequency-domain interferometer. Because of the chirp, temporal evolution of the optical Kerr response in CS(2) is projected into difference phase spectra. The chirped continuum shows spectral shifts that are due to induced phase modulation even when the continuum has a flat spectrum.

Frequency-domain interferometer for femtosecond time-resolved phase spectroscopy.

A new femtosecond time-resolved interferometer was developed that utilizes interference fringes in the frequency domain to obtain simultaneously difference phase spectra (DPS) and difference transmission spectra with a multichannel spectrometer. For the first time to our knowledge, transient oscillations were observed in DPS and the spectral shift of a probe pulse was time resolved together with the rise in DPS, which is clear evidence for induced phase modulation in absorptive materials.

Application of improved coupling assay method for peroxidase of diseased thyroids: report of three cases.

Recently we have developed an assay method for peroxidase-catalyzed coupling of iodotyronine residues of thyroglobulin, which is applicable to human diseased thyroid tissues. In the present study, the assay method as well as usual peroxidase assay methods were applied to thyroids of three patients (No. 1: familial goiter with impaired thyroglobulin synthesis, No. 2: mild chronic thyroiditis, No. 3: dyshormonogenetic goiter) who showed organification of iodine with high TSH levels and low thyroid hormone levels in sera. In general, these patients showed relatively high activities measured by guaiacol oxidation assay, iodide oxidation and coupling assay compared with those of control thyroids. Iodothyronine content in thyroglobulin was very low except thyroxine in No. 2. These results indicate that factors other than peroxidase may be responsible for the cause of the hypothyroid state. The coupling assay method used here is therefore useful for the detection of the 'coupling defect' in patients in a hypothyroid state.